/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 152 Two blocks \(A\) and \(B\), each... [FREE SOLUTION] | 91Ó°ÊÓ

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Two blocks \(A\) and \(B\), each of mass \(m,\) are supported as shown by three springs of the same constant \(k\) Blocks \(A\) and \(B\) are connected by a dashpot and block \(B\) is connected to the ground by two dashpots, each dashpot having the same coefficient of damping \(c\). Block \(A\) is subjected to a force of magnitude \(P=P_{m} \sin \omega_{f} t .\) Write the differential equations defining the displacements \(x_{A}\) and \(x_{B}\) of the two blocks from their equilibrium positions.

Short Answer

Expert verified
Find differential equations: 1. Block A: \( m\ddot{x}_A + c(\dot{x}_A - \dot{x}_B) + k(x_A - x_B) = P_m \sin \omega_f t \). 2. Block B: \( m\ddot{x}_B + c(\dot{x}_B - \dot{x}_A) + 2c\dot{x}_B + k(x_B - x_A) + 2kx_B = 0 \)."

Step by step solution

01

Identify Forces on Block A

Block A is subjected to three forces: a spring force from block B, a damping force from the dashpot connecting A and B, and the external force. The spring force exerted by the spring between block A and B is \[ F_{spring, A} = k(x_B - x_A) \]. The damping force is \[ F_{damp, A} = c(\dot{x}_B - \dot{x}_A) \], and the external force is given by \[ F_{ext} = P_m \sin \omega_f t \]. Newton's second law gives us the equation for block A as \[ m\ddot{x}_A = k(x_B - x_A) + c(\dot{x}_B - \dot{x}_A) + P_m \sin \omega_f t \].
02

Sum of Forces on Block B

Block B is affected by four forces: the spring force from block A, damping forces from the dashpot connecting A and B, two damping forces from the dashpots to the ground, and spring forces from the springs to the ground. The spring force is \[ F_{spring, B} = -k(x_B - x_A) \]. The damping force from the connection to block A is \[ F_{damp, B1} = -c(\dot{x}_B - \dot{x}_A) \]. The damping forces from the dashpots to the ground are \[ 2c\dot{x}_B \]. The spring forces from the springs to the ground are \[ 2kx_B \]. Summing these, we apply Newton's second law: \[ m\ddot{x}_B = -k(x_B - x_A) - c(\dot{x}_B - \dot{x}_A) - 2c\dot{x}_B - 2kx_B \].
03

Derive the Differential Equations

Using the forces calculated in the previous steps, combine them into the differential equations for each block: For block A, the differential equation is \[ m\ddot{x}_A + c(\dot{x}_A - \dot{x}_B) + k(x_A - x_B) = P_m \sin \omega_f t \].For block B, it becomes\[ m\ddot{x}_B + c(\dot{x}_B - \dot{x}_A) + 2c\dot{x}_B + k(x_B - x_A) + 2kx_B = 0 \]. These are the required differential equations that describe the motion of each block.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Newton's Second Law
Newton's Second Law is a fundamental principle in physics that describes how the motion of an object is affected by the forces acting on it. At its core, the law states that the acceleration of an object is directly proportional to the net force acting on it and inversely proportional to its mass. Mathematically, this is expressed as \( F = ma \), where \( F \) is the net force, \( m \) is the mass of the object, and \( a \) is the acceleration.
In the context of mechanical systems with springs and damping forces, Newton's Second Law helps us set up differential equations. These equations describe the motion of objects like blocks in our exercise. For example, for Block A subjected to various forces, we use this law to equate the sum of forces to \( m\ddot{x}_A \). This includes contributions from spring forces, damping forces, and external periodic forces. By applying Newton's Second Law, we can understand how all these forces work together to influence the movement of the blocks.
Damping Force
Damping force is a type of resistance that acts opposite to the motion of an object, typically reducing its velocity. It plays a crucial role in systems where energy dissipation is desired or naturally occurs, like in shock absorbers. The standard mathematical expression for damping force in a linear system is \( F_{damping} = -c\dot{x} \), where \( c \) is the damping coefficient and \( \dot{x} \) is the velocity.- **Understanding Damping:** - *Coefficient \( c \):* Represents the damping characteristics. A higher \( c \) means more resistance and better energy dissipation. - *Influence on Motion:* Damping affects how quickly a system returns to equilibrium or steady state.In our exercise, damping forces are considered for both blocks connecting with each other and with the ground. For instance, the dashpot's damping force between Block A and B is \( c(\dot{x}_B - \dot{x}_A) \). It serves to slow down the relative motion between the blocks, therefore affecting how force and motion transfer across the system.
Spring Constant
The spring constant, denoted as \( k \), describes how stiff a spring is. It's a measure of the force required to displace the spring by a unit distance. Formally, Hooke's Law gives us \( F_{spring} = -k x \), where \( x \) is the displacement from equilibrium. The negative sign indicates that the force exerted by the spring is always in the opposite direction of the displacement.- **Key Points about Spring Constant: ** - *Stiffness:* A larger \( k \) means a stiffer spring, which requires more force to compress or extend. - *Role in Mechanical Systems:* Springs store potential energy and help absorb and transmit forces.In mechanical systems like our two-block setup, the spring constant \( k \) helps dictate the force interactions between the masses and their vibrations. The differential equations involve terms like \( k(x_B - x_A) \), representing the force exerted by the spring on Block A due to its compression or extension.
Harmonic Oscillation
Harmonic oscillation refers to a type of periodic motion that is characterized by oscillations around an equilibrium position, influenced by restoring forces proportional to displacement. It is commonly exemplified by the motion of springs, pendulums, and circuits.In our exercise, harmonic oscillation can be visualized through the periodic external force \( P = P_m \sin \omega_f t \) applied to Block A. This force causes Block A to perform harmonic oscillations, or sinusoidal movements over time. The parameters \( P_m \) and \( \omega_f \) respectively denote the amplitude and angular frequency of the oscillations.Such oscillatory behavior is essential to understand:
  • **Amplitude (\( P_m \)):** Determines how far the block moves from its mean position.
  • **Frequency (\( \omega_f \)):** Describes how quickly the oscillations occur.
  • **Restoring Forces:** Spring and damping forces continually act to restore equilibrium, playing into the harmonic nature of the system.
Understanding harmonic oscillation ensures we can predict and analyze the time-dependent behavior of mechanical systems subjected to periodic forces.

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Most popular questions from this chapter

The bob of a simple pendulum of length \(l=40\) in. is released from rest when \(\theta=5^{\circ}\). Assuming simple harmonic motion, determine 1.6 s after release \((a)\) the angle \(\theta,(b)\) the magnitudes of the velocity and acceleration of the bob.

A small trailer and its load have a total mass of \(250 \mathrm{kg}\). The trailer is supported by two springs, each of constant \(10 \mathrm{kN} / \mathrm{m},\) and is pulled over a road, the surface of which can be approximated by a sine curve with an amplitude of \(40 \mathrm{mm}\) and a wavelength of \(5 \mathrm{m}\) (i.e., the distance between successive crests is \(5 \mathrm{m}\) and the vertical distance from crest to trough is \(80 \mathrm{mm}\) ). Determine (a) the speed at which resonance will occur, (b) the amplitude of the vibration of the trailer at a speed of \(50 \mathrm{km} / \mathrm{h}\).

A \(5-\mathrm{kg}\) uniform rod \(C D\) of length \(l=0.7 \mathrm{m}\) is welded at \(C\) to two elastic rods, which have fixed ends at \(A\) and \(B\) and are known to have a combined torsional spring constant \(K=24 \mathrm{N} \cdot \mathrm{m} / \mathrm{rad}\). Determine the period of small oscillations, if the equilibrium position of \(C D\) is \((a)\) vertical as shown, \((b)\) horizontal.

An 18 -lb block \(A\) slides in a vertical frictionless slot and is connected to a moving support \(B\) by means of a spring \(A B\) of constant \(k=8\) lb/ft. Knowing that the acceleration of the support is \(a=a_{m} \sin \omega_{j} t,\) where \(a_{m}=5\) \( \mathrm{ft} / \mathrm{s}^{2}\) and \(\omega_{f}=6\) rad/s, determine (a) the maximum displacement of block \(A,(b)\) the amplitude of the fluctuating force exerted by the spring on the block.

A \(10-\) -lb block \(A\) rests on a \(40-\) lb plate \(B\) that is attached to an unstretched spring with a constant of \(k=60\) Ib/ft. Plate \(B\) is slowly moved 2.4 in. to the left and released from rest. Assuming that block \(A\) does not slip on the plate, determine ( \(a\) ) the amplitude and frequency of the resulting motion, \((b)\) the corresponding smallest allowable value of the coefficient of static friction.

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